Anode plasma dynamics in the self-magnetic-pinch diode

The self-magnetic-pinch diode is being developed as an intense electron beam source for pulsed-power-driven x-ray radiography. In high-power operation, the beam electrons desorb contaminants from the anode surface from which positive ions are drawn to the cathode. The counterstreaming electrons and...

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Main Authors: Nichelle Bruner, Dale R. Welch, Kelly D. Hahn, Bryan V. Oliver
Format: Article
Language:English
Published: American Physical Society 2011-02-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.14.024401
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spelling doaj-42e87a2829d443b783569bd51b3ca00a2020-11-24T21:26:38ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022011-02-0114202440110.1103/PhysRevSTAB.14.024401Anode plasma dynamics in the self-magnetic-pinch diodeNichelle BrunerDale R. WelchKelly D. HahnBryan V. OliverThe self-magnetic-pinch diode is being developed as an intense electron beam source for pulsed-power-driven x-ray radiography. In high-power operation, the beam electrons desorb contaminants from the anode surface from which positive ions are drawn to the cathode. The counterstreaming electrons and ions establish an equilibrium current. It has long been recognized, however, that expanding electrode plasmas can disrupt this equilibrium and cause rapid reduction of the diode impedance and the radiation pulse. Recently developed numerical techniques, which enable simultaneous modeling of particle currents with 10^{13}  cm^{-3} densities to plasmas of near solid density, are applied to a model of the self-magnetic-pinch diode which includes the formation and evolution of anode surface plasmas. Two mechanisms are shown to cause rapid impedance loss, anode plasma expansion into the anode-cathode (A-K) gap, and increased ion space-charge near the cathode surface. The former mechanism dominates for shorter A-K gaps, while the latter dominates for longer gaps. Model results qualitatively reproduce the time-dependent impedances measured for this diode.http://doi.org/10.1103/PhysRevSTAB.14.024401
collection DOAJ
language English
format Article
sources DOAJ
author Nichelle Bruner
Dale R. Welch
Kelly D. Hahn
Bryan V. Oliver
spellingShingle Nichelle Bruner
Dale R. Welch
Kelly D. Hahn
Bryan V. Oliver
Anode plasma dynamics in the self-magnetic-pinch diode
Physical Review Special Topics. Accelerators and Beams
author_facet Nichelle Bruner
Dale R. Welch
Kelly D. Hahn
Bryan V. Oliver
author_sort Nichelle Bruner
title Anode plasma dynamics in the self-magnetic-pinch diode
title_short Anode plasma dynamics in the self-magnetic-pinch diode
title_full Anode plasma dynamics in the self-magnetic-pinch diode
title_fullStr Anode plasma dynamics in the self-magnetic-pinch diode
title_full_unstemmed Anode plasma dynamics in the self-magnetic-pinch diode
title_sort anode plasma dynamics in the self-magnetic-pinch diode
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2011-02-01
description The self-magnetic-pinch diode is being developed as an intense electron beam source for pulsed-power-driven x-ray radiography. In high-power operation, the beam electrons desorb contaminants from the anode surface from which positive ions are drawn to the cathode. The counterstreaming electrons and ions establish an equilibrium current. It has long been recognized, however, that expanding electrode plasmas can disrupt this equilibrium and cause rapid reduction of the diode impedance and the radiation pulse. Recently developed numerical techniques, which enable simultaneous modeling of particle currents with 10^{13}  cm^{-3} densities to plasmas of near solid density, are applied to a model of the self-magnetic-pinch diode which includes the formation and evolution of anode surface plasmas. Two mechanisms are shown to cause rapid impedance loss, anode plasma expansion into the anode-cathode (A-K) gap, and increased ion space-charge near the cathode surface. The former mechanism dominates for shorter A-K gaps, while the latter dominates for longer gaps. Model results qualitatively reproduce the time-dependent impedances measured for this diode.
url http://doi.org/10.1103/PhysRevSTAB.14.024401
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